/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Q1P Show that the differential equat... [FREE SOLUTION] | 91影视

91影视

Show that the differential equations for V and A (Eqs. 10.4 and 10.5) can be written in the more symmetrical form

饾啅2V+Lt=-1p饾啅2A-L=-J}

Where

饾啅22-2t2andL.A+Vt

Short Answer

Expert verified

The differential equations for V and Ain the symmetrical form are derived as

2V+t.A=-1pand2A-2At=-J

Step by step solution

01

Expression for the differential equations for V and A:

Using equation 10.6, write the differential equation for V.

饾啅2V+t=-1p 鈥︹ (1)

Here.饾啅 is d鈥 Alembertian.

Similarly, write the differential equation for A.

饾啅2A-L=-J

02

Determine the differential equations for V and A in the symmetric form:

Substitute 饾啅2=2-2t2andL=.A+Vtand in equation (1).

饾啅2-2t2V+t.A+Vt=-1p2V-2Vt2+t.A+2Vt2=-1p2V+t.A=-1p

Which is equal to the equation 10.4 as2V+t.A=-1p.

Substitute饾啅2=2-2t2andL=.A+Vtin equation (2).

2-2t2A-.A+Vt=-J2A-2At2-.A+Vt=-J

Which is equal to the equation 10.5 as .

2A-2At2-.A+Vt=-J

Therefore, the differential equations for V and Ain the symmetrical form are derived as 2V+t.A=-1pand .

2A-2At2-.A+Vt=-J

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with 91影视!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Find the (Lorenz gauge) potentials and fields of a time-dependent ideal electric dipole p(t) at the origin. (It is stationary, but its magnitude and/or direction are changing with time.) Don't bother with the contact term. [Answer:

V(r,t)=14蟺蔚0r^r2[p+(r/c)p]A(r,t)=04[]E(r,t)=04{Pr^(r^p)+c2[p+(r/c)p]3r^(r^[p+(r/c)p])r3}B(r,t)=04{r^[p+(r/c)p]r2}

Where all the derivatives of p are evaluated at the retarded time.]

In Chapter 5, I showed that it is always possible to pick a vector potential whose divergence is zero (the Coulomb gauge). Show that it is always possible to choose.A=-00(V/t), as required for the Lorenz gauge, assuming you know how to solve the inhomogeneous wave equation (Eq. 10.16). Is it always possible to pickV=0 ? How aboutA=0 ?

For a point charge moving at constant velocity, calculate the flux integralE.da (using Eq. 10.75), over the surface of a sphere centered at the present location of the charge.

Figure 2.35 summarizes the laws of electrostatics in a "triangle diagram" relating the source (), the field ,(E) and the potential (V). Figure 5.48 does the same for magnetostatics, where the source is J, the field isB , and the potential is A. Construct the analogous diagram for electrodynamics, with sources andJ (constrained by the continuity equation), fields EandB , and potentialsVandA (constrained by the Lorenz gauge condition). Do not include formulas for VandA in terms of Eandrole="math" localid="1657970465123" B .

Show that the scalar potential of a point charge moving with constant velocity (Eq. 10.49) can be written more simply as

V(r,t)=14蟺蔚0qR1-v2sin2c2 (10.51)

whereRr-vtis the vector from the present (!) position of the particle to the field point r, andis the angle between R and v (Fig. 10.9). Note that for nonrelativistic velocities (v2c2),

V(r,t)14蟺蔚0qR

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.